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Ring Resonator Design

Ring laser cavity of N curved mirrors: free spectral range, finesse, linewidth, photon lifetime, stability and the astigmatic mode sizes from the tilted mirrors.

Model: Textbook approximation

Free spectral range c/L

999.3 MHz

Finesse ℱ = π ρ^¼/(1 − √ρ)

102.4

Round-trip power factor ρ = 0.9405

Linewidth (FWHM)

9.757 MHz

Q = ν/Δν = 2.89e7

Photon lifetime

16.31 ns

Threshold round-trip gain 1/ρ = 1.063

Angle of incidence on each mirror

30.00°

Segment d = L/N = 100.0 mm

Effective radius R_t / R_s

866.0 / 1155 mm

R cos α in the ring plane, R/cos α across it

Spot on mirrors: tangential / sagittal

269.4 µm / 288.4 µm

Waist mid-segment: tangential / sagittal

261.6 / 282.1 µm

Ellipticity w_s/w_t on the mirrors 1.07

ρ = Roc(1 − loss); intracavity power ∝ 1/(1 + F sin²(πΔν/FSR)), F = 4√ρ/(1 − √ρ)²; τ = (L/c)/(−ln ρ).

Period matrix free(d)·mirror(Reff): m = 1 − d/Reff, stable for |m| < 1, spot on the mirror w² = (λd/π)/√(1 − m²). α = 90° − 180°/N.

Cavity resonances over ±1.5 FSR

0.20.40.60.81.0-1.0k-50005001.0kDetuning Δν (MHz)Intracavity power / peak
  • Intracavity power / peak

Model and references

Textbook approximation. A standard approximation from the literature (for example paraxial, plane-wave or Gaussian-beam), valid within the range the page states. About the tiers

N identical concave mirrors on a regular polygon, one output coupler. Finesse and linewidth from the Airy response of a one-way ring; modes from the paraxial period matrix with R cos α and R/cos α for the tilted mirrors. Image rotation in non-planar rings and thermal lensing are not modelled.

  1. Kogelnik H., Ippen E. P., Dienes A., Shank C. V. (1972). Astigmatically compensated cavities for CW dye lasers. IEEE J. Quantum Electron. 8, 373–379. doi:10.1109/jqe.1972.1076964
  2. Kogelnik H., Li T. (1966). Laser beams and resonators. Appl. Opt. 5, 1550–1567. doi:10.1364/ao.5.001550
  3. Siegman A. E. (1986). Lasers, ch. 11 and 21. University Science Books.
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